TWI612722B - Lte multiband monopole antenna used in electronic appliance having metal frame - Google Patents

Lte multiband monopole antenna used in electronic appliance having metal frame Download PDF

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TWI612722B
TWI612722B TW105128975A TW105128975A TWI612722B TW I612722 B TWI612722 B TW I612722B TW 105128975 A TW105128975 A TW 105128975A TW 105128975 A TW105128975 A TW 105128975A TW I612722 B TWI612722 B TW I612722B
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antenna
mode
shaped
metal frame
frequency
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TW201810800A (en
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潘建源
方穎昇
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國立高雄應用科技大學
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Abstract

本發明係有關於一種應用於具有金屬邊框之電子裝置的LTE多頻單極天線,係包括接地元件、天線元件及金屬邊框部;接地元件位於基板的第一表面,天線元件位於相對基板之第一表面的第二表面,金屬邊框部位於基板的周邊;天線元件包括第一輻射單元及第二輻射單元,第一輻射單元連接一電路元件組,天線訊號由第一輻射單元饋入,第二輻射單元由接地元件延伸,其一端連接一垂直於金屬邊框部之第一L形金屬部,第二輻射單元的另一端以一電感元件連接C型延伸部。本發明之天線在返回損失6 dB以下,可操作在低頻操作頻寬為273 MHz (687-960 MHz),平均增益為0.8 dB (0.2-1.4 dBi),平均效率約為46.75% (42-53%);高頻操作頻寬為1021 MHz (1675-2696 MHz),平均增益為3.78 dB (3.4-4.3 dBi),平均效率為77.56% (70-85%),本發明天線可以應用於LTE700/GSM850/900 (704-960 MHz)及GSM1800/1900/UMTS/LTE2300/2500 (1710-2690 MHz)之頻帶。The invention relates to an LTE multi-frequency monopole antenna applied to an electronic device with a metal frame, comprising a grounding element, an antenna element and a metal frame part; the grounding element is located on the first surface of the substrate, and the antenna element is located on the opposite substrate a second surface of a surface, the metal frame portion is located at a periphery of the substrate; the antenna element includes a first radiating unit and a second radiating unit, the first radiating unit is connected to a circuit component group, and the antenna signal is fed by the first radiating unit, and the second The radiating unit is extended by the grounding member, one end of which is connected to a first L-shaped metal portion perpendicular to the metal frame portion, and the other end of the second radiating unit is connected to the C-shaped extending portion by an inductive element. The antenna of the present invention has a return loss of less than 6 dB, operates at a low frequency operating bandwidth of 273 MHz (687-960 MHz), has an average gain of 0.8 dB (0.2-1.4 dBi), and an average efficiency of approximately 46.75% (42-53). %); the high frequency operating bandwidth is 1021 MHz (1675-2696 MHz), the average gain is 3.78 dB (3.4-4.3 dBi), and the average efficiency is 77.56% (70-85%). The antenna of the present invention can be applied to LTE700/ Bands for GSM850/900 (704-960 MHz) and GSM1800/1900/UMTS/LTE2300/2500 (1710-2690 MHz).

Description

應用於具有金屬邊框之電子裝置的LTE多頻單極天線LTE multi-frequency monopole antenna for electronic devices with metal frame

本發明係有關於一種單極天線,尤其是指一種應用於具有金屬邊框之電子裝置的LTE多頻單極天線。The present invention relates to a monopole antenna, and more particularly to an LTE multi-frequency monopole antenna applied to an electronic device having a metal frame.

隨著行動通訊產業的快速發展,現今無線傳輸介面已逐漸由第三代(3G)行動通信系統進化到第四代(4G)行動通信系統,而長期演進技術(Long Term Evolution, LTE)就是第四代行動通信系統中的其中一種通信協定。With the rapid development of the mobile communication industry, today's wireless transmission interface has gradually evolved from the third generation (3G) mobile communication system to the fourth generation (4G) mobile communication system, and Long Term Evolution (LTE) is the first One of the communication protocols in the four-generation mobile communication system.

人們對於行動通訊裝置的需求愈來愈多元化,為了滿足使用者的需求,業者將更多元件置入行動通訊裝置,然而此舉勢必會壓縮到天線的設計空間。The demand for mobile communication devices is becoming more and more diversified. In order to meet the needs of users, more components are placed in mobile communication devices, but this will inevitably be compressed into the design space of the antenna.

尤其近年來,行動通訊裝置的顯示螢幕朝大尺寸方向發展,使得顯示螢幕與行動通訊裝置機殼之頂部和底部邊緣之間的區域變得非常窄,通常會小於10 mm,而行動通訊裝置的天線就是設計在此區域。In particular, in recent years, the display screen of the mobile communication device has moved toward a large size, so that the area between the display screen and the top and bottom edges of the mobile communication device casing is very narrow, usually less than 10 mm, and the mobile communication device The antenna is designed in this area.

因此,天線設計者不僅要考慮到天線效能的需求,天線也要以小尺寸為主軸,與周邊環境整合,並要能達成寬頻的頻帶操作;而天線縮小化的方向,以降低天線之高度較為重要,因此天線高度至少要低於10 mm才是目前行動通訊裝置天線設計之趨勢。Therefore, the antenna designer must not only consider the requirements of the antenna performance, but also the antenna should be small-sized as the main axis, integrated with the surrounding environment, and can achieve broadband frequency band operation; and the antenna is reduced in direction to reduce the height of the antenna. Important, so an antenna height of at least 10 mm is the current trend in antenna design for mobile communication devices.

此外,先前行動通訊裝置之機殼大部分都是使用塑膠材質製作,由於行動通訊裝置也同時朝向薄型化發展,導致塑膠材質製成的機殼的機械強度不足,於是行動通訊裝置業者改以金屬材質作為行動通訊裝置的背蓋或邊框上的材質,用以提高行動通訊裝置之機械強度,甚至透過金屬材質的背蓋或邊框使行動通訊裝置的外觀得以美型化,並提升整體質感,尤其是高規格行動通訊裝置。In addition, most of the casings of the previous mobile communication devices were made of plastic materials. As the mobile communication device was also thinner, the mechanical strength of the casing made of plastic material was insufficient, so the mobile communication device was changed to metal. The material is used as the material of the back cover or the frame of the mobile communication device to improve the mechanical strength of the mobile communication device, and even the metal back cover or the frame can make the appearance of the mobile communication device beautiful and improve the overall texture, especially It is a high specification mobile communication device.

而使用了金屬背蓋或者是邊框的行動通訊裝置,雖能讓行動通訊裝置的機械強度因此隨之提升,但卻使天線設計的環境更加艱難,因此,在行動通訊裝置顯示螢幕與金屬邊框之間可用的區域下設計一款滿足LTE系統多頻帶天線並有良好的輻射特性之天線是目前一大挑戰。The use of a metal back cover or a framed mobile communication device can increase the mechanical strength of the mobile communication device, but the antenna design environment is more difficult. Therefore, the mobile communication device displays the screen and the metal frame. It is currently a challenge to design an antenna that satisfies the multi-band antenna of the LTE system and has good radiation characteristics under the available area.

<引用文獻><Citations>

文獻1:US 8547283 B2Document 1: US 8547283 B2

文獻2:US 20110095949 A1Document 2: US 20110095949 A1

文獻3:TW I488361Document 3: TW I488361

文獻4:TW I509883Document 4: TW I509883

文獻5:J. H. Lu and J. L. Guo, “Small-Size Octaband Monopole Antenna in an LTE/WWAN Mobile Phone,” IEEE Antennas and Wireless Propag. Lett.,vol.13, pp.548-551, 2014. Document 5: JH Lu and JL Guo, "Small-Size Octaband Monopole Antenna in an LTE/WWAN Mobile Phone," IEEE Antennas and Wireless Propag. Lett. , vol. 13, pp. 548-551, 2014.

文獻6:S. C. Chen and K. L. Wong, “Small-Size Wideband Chip Antenna For WWAN/LTE Operation and Close Integration with Nearby Conducting Elements in the Mobile Handset,” Microwave Opt. Technol. Lett., vol.53, no.9, pp.1998-2004, Sep. 2011. Document 6: SC Chen and KL Wong, "Small-Size Wideband Chip Antenna For WWAN/LTE Operation and Close Integration with Nearby Conducting Elements in the Mobile Handset," Microwave Opt. Technol. Lett. , vol.53, no.9, Pp.1998-2004, Sep. 2011.

文獻7:S. C. Chen and K. L. Wong, “Wideband Monopole Antenna Coupled with a Chip-Inductor-loaded Shorted Strip for LTE/WWAN Mobile Handset,” Microwave Opt. Technol. Lett., vol.53, no.6, pp.1293-1298, Jun. 2011. Document 7: SC Chen and KL Wong, “Wideband Monopole Antenna Coupled with a Chip-Inductor-loaded Shorted Strip for LTE/WWAN Mobile Handset,” Microwave Opt. Technol. Lett. , vol.53, no.6, pp.1293 -1298, Jun. 2011.

上述各文獻,有的係揭示使用立體式結構,或者是具有天線面積較大之缺點,而仍有改善的空間,此外,上述各文獻在天線設計上均無考慮金屬材質之背蓋或者是邊框,在實際應用上會大幅影響天線特性。In the above documents, some disclose the use of a three-dimensional structure, or have the disadvantage of having a large antenna area, and there is still room for improvement. Moreover, the above-mentioned documents do not consider the back cover or the frame of the metal material in the antenna design. In practical applications, the antenna characteristics will be greatly affected.

本發明之主要目的,係提供一種天線,特別是應用在具有金屬邊框的行動通訊裝置上,主要係設置在有限之空間上,並能達到多頻帶的操作,以滿足行動通訊裝置的需求。The main object of the present invention is to provide an antenna, particularly for use in a mobile communication device having a metal frame, which is mainly disposed in a limited space and can achieve multi-band operation to meet the needs of a mobile communication device.

本發明之目的及功效,係由以下技術實現:The object and effect of the present invention are achieved by the following techniques:

一種應用於具有金屬邊框之電子裝置的LTE多頻單極天線;至少包含一接地元件、一天線元件及一金屬邊框部;An LTE multi-frequency monopole antenna applied to an electronic device having a metal frame; comprising at least one grounding element, an antenna element and a metal frame portion;

所述接地元件位於一基板的第一表面,相對所述第一表面的所述基板的第二表面上設所述天線元件,所述金屬邊框部位於所述基板的周邊;The grounding element is located on a first surface of a substrate, and the antenna element is disposed on a second surface of the substrate opposite to the first surface, the metal frame portion is located at a periphery of the substrate;

所述天線元件包含第一輻射單元及第二輻射單元;所述第一輻射單元包括彼此連接延伸的一電路元件組以及一L形延伸部,所述L形延伸部遠離所述電路元件組的一端為第一自由端;所述電路元件組包含一第一電感元件與一電容元件,所述電容元件的一端為天線訊號饋入點並與所述接地元件連接,所述電容元件的另一端連接所述第一電感元件與所述L形延伸部,所述電感元件的另一端連接所述接地元件;The antenna element includes a first radiating element and a second radiating unit; the first radiating unit includes a circuit component group extending from each other and an L-shaped extension, the L-shaped extension being remote from the circuit component group One end is a first free end; the circuit component group includes a first inductive component and a capacitive component, one end of the capacitive component is an antenna signal feed point and is connected to the ground component, and the other end of the capacitive component Connecting the first inductive component and the L-shaped extension, and connecting the other end of the inductive component to the grounding component;

所述第二輻射單元與所述接地元件連接,並至少具有C形延伸部與鉤狀延伸部,所述C形延伸部及所述鉤狀延伸部分別具有第三自由端及第四自由端,所述C形延伸部及所述鉤狀延伸部之間連接有第二電感元件,所述鉤狀延伸部設一端點與所述接地元件連接,所述鉤狀延伸部之端點與所述第四自由端之間形成開口,應用於具有金屬邊框之電子裝置的LTE多頻單極天線所述L形延伸部由所述開口深入所述鉤狀延伸部,所述鉤狀延伸部之末端和所述金屬邊框部連接,所述C形延伸部的自由端係位在所述第二輻射單元與所述接地元件連接處的一側;The second ejector unit is coupled to the grounding element and has at least a C-shaped extension and a hook-shaped extension, the C-shaped extension and the hook-shaped extension having a third free end and a fourth free end, respectively a second inductive component is connected between the C-shaped extension and the hook-shaped extension, and the hook-shaped extension is provided with an end point connected to the grounding element, and an end point of the hook-shaped extension Forming an opening between the fourth free ends, applied to an LTE multi-frequency monopole antenna having a metal frame electronic device, wherein the L-shaped extension portion penetrates the hook-shaped extension portion from the opening, and the hook-shaped extension portion The end is connected to the metal frame portion, and the free end of the C-shaped extension is tied to a side of the junction of the second radiation unit and the ground element;

所述金屬邊框部包括第一L形金屬部、第二L形金屬部及U形金屬部,所述第一L形金屬部、所述第二L形金屬部及所述U形金屬部係包圍設置在所述基板周圍。The metal frame portion includes a first L-shaped metal portion, a second L-shaped metal portion, and a U-shaped metal portion, the first L-shaped metal portion, the second L-shaped metal portion, and the U-shaped metal portion The surround is disposed around the substrate.

如上所述之應用於具有金屬邊框之電子裝置的LTE多頻單極天線,其中,所述第二輻射單元自與所述接地元件連接之端點至所述第四自由端之路徑,再經由連接的所述第一L形金屬部之第二自由端以激發出第一模態。An LTE multi-frequency monopole antenna applied to an electronic device having a metal frame as described above, wherein the second radiating element is from a terminal connected to the ground element to a path of the fourth free end, and then A second free end of the first L-shaped metal portion is coupled to excite the first mode.

如上所述之應用於具有金屬邊框之電子裝置的LTE多頻單極天線,其中,所述第二輻射單元延伸自與所述接地元件連接之端點至所述C形延伸部之第三自由端之路徑以激發出第二模態。An LTE multi-frequency monopole antenna applied to an electronic device having a metal frame as described above, wherein the second radiating element extends from an end point connected to the ground element to a third freedom of the C-shaped extension The path of the end to excite the second mode.

如上所述之應用於具有金屬邊框之電子裝置的LTE多頻單極天線,其中,所述饋入點至第一電感元件連接所述接地元件之路徑以激發出第三模態。The LTE multi-frequency monopole antenna applied to an electronic device having a metal frame as described above, wherein the feeding point to the first inductive element connects the path of the ground element to excite the third mode.

如上所述之應用於具有金屬邊框之電子裝置的LTE多頻單極天線,其中,所述第二輻射單元延伸自所述接地元件之端點至第四自由端之路徑再經由連接的所述第一L形金屬部之第二自由端以激發出第四模態,所述第四模態之頻率為所述第一模態之頻率的三倍。An LTE multi-frequency monopole antenna applied to an electronic device having a metal frame as described above, wherein the second radiating element extends from a path of an end of the ground element to a path of a fourth free end and then via the connection A second free end of the first L-shaped metal portion excites a fourth mode, the fourth mode having a frequency that is three times the frequency of the first mode.

如上所述之應用於具有金屬邊框之電子裝置的LTE多頻單極天線,其中,所述第二輻射單元延伸自所述接地元件之端點至所述C形延伸部之第三自由端之路徑以激發出第五模態,所述第五模態之頻率為所述第一模態之頻率的三倍。An LTE multi-frequency monopole antenna applied to an electronic device having a metal frame as described above, wherein the second radiating element extends from an end of the ground element to a third free end of the C-shaped extension The path is to excite a fifth mode, the fifth mode having a frequency that is three times the frequency of the first mode.

如上所述之應用於具有金屬邊框之電子裝置的LTE多頻單極天線,其中,由所述饋入點至所述第一自由端之路徑以激發出第六模態。An LTE multi-frequency monopole antenna applied to an electronic device having a metal frame as described above, wherein a path from the feed point to the first free end excites a sixth mode.

如上所述之應用於具有金屬邊框之電子裝置的LTE多頻單極天線,其中,所述第一模態、所述第二模態及所述第三模態共同涵蓋687 MHz至960 MHz頻帶,所述第四模態、所述第五模態及所述第六模態共同涵蓋1675 MHz至2696 MHz頻帶。An LTE multi-frequency monopole antenna applied to an electronic device having a metal frame as described above, wherein the first mode, the second mode, and the third mode collectively cover a band of 687 MHz to 960 MHz The fourth mode, the fifth mode, and the sixth mode collectively cover the 1675 MHz to 2696 MHz band.

如上所述之應用於具有金屬邊框之電子裝置的LTE多頻單極天線,其中,所述第一L形金屬部與所述第二L形金屬部對應,所述U形金屬部的二端分別與所述第一L形金屬部、所述第二L形金屬部相鄰且各形成一第一間距、第二間距,所述第一間距、第二間距距離相等,所述第一L形金屬部與所述第二L形金屬部間形成第三間距。An LTE multi-frequency monopole antenna applied to an electronic device having a metal frame as described above, wherein the first L-shaped metal portion corresponds to the second L-shaped metal portion, and the two ends of the U-shaped metal portion Forming a first pitch and a second pitch respectively adjacent to the first L-shaped metal portion and the second L-shaped metal portion, wherein the first pitch and the second pitch are equal, the first L A third spacing is formed between the shaped metal portion and the second L-shaped metal portion.

本創作之天線因其第一模態、第二模態及第三模態共同涵蓋687 MHz至960 MHz頻帶;第四模態、第五模態及第六模態共同涵蓋1675 MHz至2696 MHz頻帶,因此可應用於行動通訊裝置之天線裝置上;此外,本發明之天線面積大約為30 × 8 mm 2,相較於目前可涵蓋上述八個頻帶的先前技術而言,本發明之天線面積可縮減超過20%以上。 The antenna of this creation covers the band 687 MHz to 960 MHz for its first mode, second mode and third mode; the fourth mode, the fifth mode and the sixth mode together cover 1675 MHz to 2696 MHz. The frequency band is therefore applicable to the antenna device of the mobile communication device; in addition, the antenna area of the present invention is approximately 30 × 8 mm 2 , which is the antenna area of the present invention compared to the prior art which currently covers the above eight frequency bands. Can be reduced by more than 20%.

承上所述,本發明之應用於具有金屬邊框之電子裝置的LTE多頻單極天線,其優點為:In view of the above, the LTE multi-frequency monopole antenna of the present invention applied to an electronic device having a metal frame has the following advantages:

1.本天線可藉由第一輻射單元、第二輻射單元之設計,相較於先前所發表相關文獻應用在相同之頻帶可縮小天線所需要的面積,以滿足行動通訊裝置之需求。1. The antenna can be designed by the first radiating element and the second radiating element, and the area required for the antenna can be reduced in the same frequency band as the previously published related documents to meet the requirements of the mobile communication device.

2.本天線元件利用電子裝置的金屬邊框部與天線元件結合,將金屬邊框部納入天線輻射體之一,可以有效的整合行動通訊裝置天線周圍環境。2. The antenna element is combined with the antenna element by the metal frame portion of the electronic device, and the metal frame portion is incorporated into one of the antenna radiators, so that the environment around the antenna of the mobile communication device can be effectively integrated.

3.本天線由實施例之各項實驗測量數據可知,在大範圍的操作頻帶內皆能維持良好的輻射特性。3. This antenna is based on the experimental measurements of the examples, and it is known that good radiation characteristics can be maintained in a wide operating band.

為令本發明所運用之技術內容、發明目的及其達成之功效有更完整且清楚的揭露,茲於下詳細說明之,並請一併參閱所揭之圖式及圖號:For a more complete and clear disclosure of the technical content, the purpose of the invention and the effects thereof achieved by the present invention, it is explained in detail below, and please refer to the drawings and drawings:

請參看第一、二圖,係揭示本發明之應用於具有金屬邊框之電子裝置的LTE多頻單極天線的一較佳實施例,此天線至少包含接地元件(1)、天線元件(2)、金屬邊框部(3);其中:Please refer to the first and second figures for revealing a preferred embodiment of the LTE multi-frequency monopole antenna applied to an electronic device having a metal frame, the antenna comprising at least a grounding component (1) and an antenna component (2) , metal frame part (3); where:

接地元件(1)設置於一基板(4)的第一表面(41),該基板(4)還包括相對第一表面(41)的第二表面(42),於第二表面(42)的上方右側形成有淨空區(421)。The grounding element (1) is disposed on the first surface (41) of the substrate (4), the substrate (4) further comprising a second surface (42) opposite to the first surface (41) on the second surface (42) A clearance area (421) is formed on the upper right side.

天線元件(2)係以印刷、蝕刻、金屬片沖壓或切割等方式設置於基板(4)之第二表面(42),且是第二表面(42)上的淨空區(421)。The antenna element (2) is disposed on the second surface (42) of the substrate (4) by printing, etching, sheet metal stamping or cutting, and is a clearance area (421) on the second surface (42).

天線元件(2)至少包含設置於基板(4)第一表面(41)之第一輻射單元(21)、第二輻射單元(22)。The antenna element (2) includes at least a first radiating element (21) and a second radiating element (22) disposed on the first surface (41) of the substrate (4).

第一輻射單元(21)包括有電路元件組(211)、L形延伸部(212)饋入點(A)及第一自由端(D),其中電路元件組(211)包含第一電感元件(L1)及電容元件(C1),饋入點(A)電性連接接地元件(1)並串聯電容元件C1後並聯第一電感元件(L1),第一電感元件(L1)的另一端點(B)連接接地元件(1);電容元件C1與第一電感元件(L1)組成一高通匹配電路。The first radiating element (21) includes a circuit component group (211), an L-shaped extension (212) feed point (A), and a first free end (D), wherein the circuit component group (211) includes the first inductance component (L1) and the capacitive element (C1), the feed point (A) is electrically connected to the ground element (1) and the capacitor element C1 is connected in series, and then the first inductance element (L1) is connected in parallel, and the other end point of the first inductance element (L1) (B) Connecting the grounding element (1); the capacitive element C1 and the first inductive component (L1) form a high-pass matching circuit.

第二輻射單元(22)經由接點(C)延伸自接地元件(1),且第二輻射單元(22)至少具有鉤狀延伸部(221)、C形延伸部(222)。其中,鉤狀延伸部(221)及C形延伸部(222)之間有第二電感元件(L2)連接。The second radiating element (22) extends from the grounding element (1) via a joint (C), and the second radiating element (22) has at least a hook-like extension (221) and a C-shaped extension (222). The second inductive element (L2) is connected between the hook extension (221) and the C-shaped extension (222).

金屬邊框部(3)由垂直於基板(4)之第一L形金屬部(31)、第二L形金屬部(32)及U形金屬部(33)組成,其中,第一L形金屬部(31)與第二輻射單元(22)之鉤狀延伸部(221)之末端連接,第二L形金屬部(32)及U形金屬部(33)與接地元件(1)連接,而第一L形金屬部(31)與第二L形金屬部(32)之間具有間距W,第一L形金屬部(31)與U形金屬部(33)之間具有間距d1,第二L形金屬部(32)與U形金屬部(33)之間具有間距d2,其中間距d1與間距d2相等。The metal frame portion (3) is composed of a first L-shaped metal portion (31) perpendicular to the substrate (4), a second L-shaped metal portion (32) and a U-shaped metal portion (33), wherein the first L-shaped metal portion The portion (31) is connected to the end of the hook-like extension (221) of the second radiating element (22), and the second L-shaped metal portion (32) and the U-shaped metal portion (33) are connected to the grounding member (1), and The first L-shaped metal portion (31) has a spacing W between the second L-shaped metal portion (32), and the first L-shaped metal portion (31) and the U-shaped metal portion (33) have a spacing d1, and a second The L-shaped metal portion (32) and the U-shaped metal portion (33) have a spacing d2, wherein the spacing d1 is equal to the spacing d2.

此外,第一輻射單元(21)之L形延伸部(212)遠離饋入點(A)的一端為第一自由端(D);第二輻射單元(22)之鉤狀延伸部(221)、C形延伸部(222)的末端分別為第四自由端(H)及第三自由端(F);第一L形金屬部(31)遠離與鉤狀延伸部(221)連接的一端為第二自由端(E)。其中,饋入點(A)至第一自由端(D)形成饋入帶單極路徑(AD),接點(C)至第二自由端(E)形成寄生短路之長路徑(CE),接點(C)至第三自由端(F)形成寄生短路之短路徑(CF);在低頻部分主要由寄生短路之長路徑(CE)以及寄生短路之短路徑(CF)各別所產生共振模態,再加入饋入點(A)以電容元件C1、第一電感元件(L1)組成的高通匹配電路所含蓋之;高頻部分則是由寄生短路之長路徑(CE)以及寄生短路之短路徑(CF)之倍頻含蓋其操作頻帶;至於饋入帶單極路徑(AD),則提供其他路徑所需要之耦合量,以調整阻抗匹配;為寄生短路之短路徑(CF)尾端與淨空區(421)邊界之間具有間距(G)。In addition, one end of the L-shaped extension (212) of the first radiating element (21) away from the feeding point (A) is a first free end (D); a hook-shaped extension of the second radiating element (22) (221) The ends of the C-shaped extensions (222) are respectively a fourth free end (H) and a third free end (F); the end of the first L-shaped metal portion (31) away from the hook-shaped extension (221) is Second free end (E). Wherein, the feeding point (A) to the first free end (D) form a feeding path unipolar path (AD), and the contact point (C) to the second free end (E) form a long path (CE) of a parasitic short circuit, The short path (CF) of the parasitic short circuit is formed from the contact point (C) to the third free end (F); the resonance mode is mainly generated by the long path (CE) of the parasitic short circuit and the short path (CF) of the parasitic short circuit in the low frequency part State, then add the feed point (A) covered by the high-pass matching circuit composed of the capacitive element C1 and the first inductance element (L1); the high-frequency part is the long path (CE) of the parasitic short circuit and the parasitic short circuit The short-path (CF) multiplier covers its operating frequency band; as for the feed-in unipolar path (AD), the coupling amount required for other paths is provided to adjust the impedance matching; the short path (CF) tail for the parasitic short circuit There is a spacing (G) between the end and the boundary of the clearance area (421).

以下就實際製作之單極天線實施例進一步針對該單極天線表面電流、結構、路徑參數進行實驗測量及理論模擬,表1揭示本發明之單極天線之最佳路徑參數值。The actual fabrication of the monopole antenna embodiment is further experimentally measured and theoretically simulated for the surface current, structure, and path parameters of the monopole antenna. Table 1 discloses the optimum path parameter values of the monopole antenna of the present invention.

表3.1 本發明之單極天線之最佳路徑參數值 <TABLE border="1" borderColor="#000000" width="85%"><TBODY><tr><td> 參數 </td><td> L<sub>1</sub></td><td> L<sub>2</sub></td><td> C<sub>1</sub></td><td> G </td></tr><tr><td> 設計值 </td><td> 8.2 nH </td><td> 10 nH </td><td> 3.3 pF </td><td> 0.5 mm </td></tr></TBODY></TABLE>Table 3.1 Optimal path parameter values of the monopole antenna of the present invention         <TABLE border="1" borderColor="#000000" width="85%"><TBODY><tr><td> Parameters</td><td> L<sub>1</sub></td> <td> L<sub>2</sub></td><td> C<sub>1</sub></td><td> G </td></tr><tr><td> Design value </td><td> 8.2 nH </td><td> 10 nH </td><td> 3.3 pF </td><td> 0.5 mm </td></tr></TBODY> </TABLE>

本天線之較佳實施例選擇下列尺寸來進行實驗測量結果及理論模擬結果:接地元件(1)之面積約為120 × 65 mm 2,天線元件(2)設置範圍的區域面積為30 × 8 mm 2;基板(4)採用厚度為0.8 mm之玻璃纖維介質基板(介電係數約為4.4),天線元件(2)則採用厚度為0.02 mm之銅片,第一L形金屬部(31)、第二L形金屬部(32)及U形金屬部(33)所組成之金屬邊框皆採用厚度為0.2 mm之銅片。 The preferred embodiment of the antenna selects the following dimensions 來 for experimental measurement results and theoretical simulation results: the area of the ground element (1) is approximately 120 × 65 mm 2 , and the area of the antenna element (2) is 30 × 8 mm 2 ; the substrate (4) is made of a glass fiber dielectric substrate with a thickness of 0.8 mm (dielectric coefficient is about 4.4), and the antenna element (2) is made of copper with a thickness of 0.02 mm, the first L-shaped metal portion (31), The metal frame composed of the second L-shaped metal portion (32) and the U-shaped metal portion (33) is made of a copper sheet having a thickness of 0.2 mm.

饋入點(A)至第一自由端(D)之路徑約為29.2 mm;由接點C經第四自由端(H)到第二自由端(E)之路徑約為62.1 mm,形成寄生短路之長路徑;由接點C到第三自由端(F)之路徑約為47.5 mm,形成寄生短路之短路徑。The path from the feed point (A) to the first free end (D) is about 29.2 mm; the path from the contact C through the fourth free end (H) to the second free end (E) is about 62.1 mm, forming a parasitic The long path of the short circuit; the path from the junction C to the third free end (F) is about 47.5 mm, forming a short path of parasitic short circuit.

請參看第三圖為本發明之應用於LTE多頻金屬邊框單極天線之較佳實施例之返回損失圖,其縱軸為返回損失值,單位為dB;橫軸為操作頻率,單位為MHz。其中,實線為理論模擬結果,實線具圓點為實驗測量結果。由第三圖可知,本發明以反射損失值大於6 dB為標準,得知其操作頻率範圍低頻部分介於687-960 MHz,低頻操作頻寬為273 MHz,頻寬百分比約為33.1 %;而高頻部分介於1675-2696 MHz,高頻操作頻寬為1021 MHz,頻寬百分比約為46.7 %;本發明之單極天線可以滿足LTE700/GSM850/900 (704 MHz至960 MHz)及GSM1800/1900/UMTS/LTE2300/2500 (1710 MHz至2690 MHz)之頻操作需求。Please refer to the third figure for the return loss diagram of the preferred embodiment of the LTE multi-frequency metal frame monopole antenna. The vertical axis is the return loss value in dB; the horizontal axis is the operating frequency in MHz. . Among them, the solid line is the theoretical simulation result, and the solid line has the dot as the experimental measurement result. As can be seen from the third figure, the present invention has a reflection loss value greater than 6 dB as a standard, and the low frequency portion of the operating frequency range is 687-960 MHz, and the low frequency operation bandwidth is 273 MHz, and the bandwidth percentage is about 33.1%; The high frequency part is between 1675 and 2696 MHz, the high frequency operation bandwidth is 1021 MHz, and the bandwidth percentage is about 46.7 %. The monopole antenna of the present invention can satisfy LTE700/GSM850/900 (704 MHz to 960 MHz) and GSM1800/ Frequency operation requirements for 1900/UMTS/LTE2300/2500 (1710 MHz to 2690 MHz).

在本天線較佳實施例中,該收發天線訊號之傳遞路徑有三條,並可對應產生五個激發模態,以及一個由第一電感元件(L1)激發之模態:In the preferred embodiment of the antenna, the transmitting and receiving antenna signals have three transmission paths, and correspondingly generate five excitation modes, and a mode excited by the first inductance element (L1):

一、第一激發模態725 MHz:經由寄生短路之長路徑(CE)所激發;First, the first excitation mode is 725 MHz: excited by the long path (CE) of the parasitic short circuit;

二、第二激發模態809 MHz:經由寄生短路之短路徑(CF)所激發;Second, the second excitation mode 809 MHz: excited by a short path (CF) of the parasitic short circuit;

三、第三激發模態906 MHz:由饋入點(A)經第一電感元件(L1)至端點B連接接地元件(1)之路徑而激發出;Third, the third excitation mode 906 MHz: is excited by the feeding point (A) through the path of the first inductive component (L1) to the end point B connected to the grounding component (1);

四、第四激發模態2031 MHz:路徑與第一激發模態相同,是第一激發模態頻率之三倍;Fourth, the fourth excitation mode 2031 MHz: the path is the same as the first excitation mode, which is three times the frequency of the first excitation mode;

五、第五激發模態2334 MHz:路徑與第二激發模態相同,是第二激發模態頻率之三倍;5. The fifth excitation mode is 2334 MHz: the path is the same as the second excitation mode, which is three times the frequency of the second excitation mode;

六、第六激發模態2600 MHz:由饋入帶單極路徑(AD)所激發。Sixth, sixth excitation mode 2600 MHz: excited by the feedthrough unipolar path (AD).

第四圖所示,為本發明之單極天線結構模擬反射損失圖。Antenna-1是未加入寄生短路之長路徑(CE),可以發現低頻帶阻抗頻寬不足以含蓋低頻操作頻帶,由此可得知寄生短路之長路徑(CE)可以在低頻共振一模態,貢獻低頻帶阻抗頻寬,高頻帶部分阻抗頻寬亦有被影響,因高頻帶有此模態之倍頻貢獻阻抗頻寬,後續會觀察輸入阻抗圖進行結構探討之共振模態證明。Antenna-2是未加入寄生短路之短路徑(CF),低頻帶阻抗匹配約只有4 dB,即可證明寄生短路之短路徑(CF)可以在低頻共振另一模態,貢獻低頻帶阻抗頻寬,高頻帶約2550 MHz之模態亦由此路徑所貢獻。Antenna-3是未加入LC高通匹配電路,發現此匹配電路對於低頻帶的阻抗頻寬是有較大的貢獻,同時對於高頻帶影響是較小的,首先參考第五圖為Antenna-1模擬輸入阻抗圖,如第五圖(a)頻率響應圖中,寄生短路之長路徑(CE)可約在700 MHz共振主模態以及2100 MHz共振倍頻模態,觀察第五圖(b)與(c)史密斯圖,Antenna-1在低頻操作頻帶內有共振一模態,但輸入阻抗尚未匹配;高頻部分則是有產生兩個共振模態,接著參考第六圖Antenna-2模擬輸入阻抗圖,第六圖(a)頻率響應,寄生短路之短路徑(CF)可約在850 MHz共振主模態以及2550 MHz共振倍頻模態,觀察第六圖(b)與(c)史密斯圖,Antenna-2在低頻帶已經有寄生短路之長路徑(CE)及LC高通匹配電路所共振之模態,但模態輸入阻抗分佈尚未在VSWR=3之範圍內,最後參考第七圖Antenna-3模擬輸入阻抗圖,第七圖(a)頻率響應中可以證明LC高通匹配電路可以在1200 MHz,主要是因為從饋入點(A)經由第一電感元件(L1)接地可以在低頻共振一高阻抗模態,藉由此模態可以將低頻帶實部阻抗提升,此外饋入點(A)串聯一電容元件C1可調整低頻帶虛部阻抗,以達到阻抗匹配,觀察第七圖(b)與(c)史密斯圖,Proposed 與Antenna-3比較之下,Antenna-3低頻帶部分確實是電容性之輸入阻抗分佈,高頻帶並沒有太大的變化,證明了LC高通匹配電路對於天線輸入阻抗等效應。The fourth figure shows a simulated reflection loss diagram of the monopole antenna structure of the present invention. Antenna-1 is a long path (CE) without parasitic short circuit. It can be found that the low-band impedance bandwidth is not enough to cover the low-frequency operating band. It can be known that the long path (CE) of the parasitic short circuit can be in the low-frequency resonance mode. The contribution of the low-band impedance bandwidth is also affected, and the high-band partial impedance bandwidth is also affected. Because the high-frequency band has the multiplier contribution impedance bandwidth of this mode, the resonance mode proof of the structure of the input impedance diagram is discussed later. Antenna-2 is a short path (CF) without parasitic short circuit. The low-band impedance matching is only about 4 dB. It can be proved that the short path (CF) of the parasitic short circuit can resonate at another mode in the low frequency and contribute the low-band impedance bandwidth. The mode of the high frequency band of about 2550 MHz is also contributed by this path. Antenna-3 is not added to the LC high-pass matching circuit. It is found that this matching circuit has a large contribution to the impedance bandwidth of the low frequency band, and the impact on the high frequency band is small. First, refer to the fifth picture for the Antenna-1 analog input. Impedance map, as shown in the fifth (a) frequency response diagram, the long path (CE) of the parasitic short circuit can be approximately 700 MHz resonant main mode and 2100 MHz resonant multiplication mode, observe the fifth figure (b) and ( c) Smith chart, Antenna-1 has a resonance mode in the low frequency operation band, but the input impedance is not matched; the high frequency part has two resonance modes, and then the sixth picture Antenna-2 analog input impedance diagram Figure 6 (a) Frequency response, the short path (CF) of the parasitic short circuit can be approximately 850 MHz resonant main mode and 2550 MHz resonant multiplication mode, observe the sixth figure (b) and (c) Smith chart, Antenna-2 has a parasitic short path (CE) in the low frequency band and a resonant mode of the LC high-pass matching circuit, but the modal input impedance distribution is not yet in the range of VSWR=3. Finally, refer to the seventh figure Antenna-3. Analog input impedance map, Figure 7 (a) Frequency response can prove LC high-pass matching The path can be at 1200 MHz, mainly because the ground can be grounded from the feed point (A) via the first inductive component (L1) to a high-impedance mode at low frequencies, whereby the low-band real impedance can be boosted by the modality. The feed point (A) is connected in series with a capacitive element C1 to adjust the low-band imaginary impedance to achieve impedance matching. Observe the seventh figure (b) and (c) Smith chart, Proposed and Antenna-3, Antenna-3 The low-band portion is indeed a capacitive input impedance distribution, and the high-frequency band does not change much, which proves the effect of the LC high-pass matching circuit on the antenna input impedance.

接著將針對Proposed Antenna進行參數探討與分析。首先固定參數:L 2= 10 nH、C 1= 3.3 pF、G = 0.5 mm,探討參數L 1為高通匹配電路之第一電感元件(L1),如第八圖參數L 1反射損失變化圖,當參數L 1在7.2 nH變化至9.2 nH的時候,由於L 1是高通匹配電路元件,電感量多寡主要影響是低頻的阻抗頻寬,也印證了前面所述高通匹配電路主要是控制低頻帶部分;接著固定參數:L 1= 8.2 nH、C 1= 3.3 pF、G = 0.5 mm,探討參數L 2為寄生短路之短路徑(CF)中之第二電感元件(L2),如第九圖參數L 2反射損失變化圖,當參數L 2在8 nH變化至12 nH,可以觀察到低頻帶第二模態之頻率會明顯的往低頻移動,寄生短路之短路徑(CF)由於加入第二電感元件(L2),得使共振波長縮短,能用較短的路徑共振在低頻帶,但電感量不宜過大,否則會影響到天線之輻射效率。固定參數:L 1= 8.2 nH、L 2= 10 nH、G = 0.5 mm,探討參數C 1為高通匹配電路之電容元件C1,如第十圖參數C 1反射損失變化圖,當參數C 1在1.3 pF變化至5.3 pF,由於電容元件C1是放置在饋入帶單極路徑(AD),因此會影響到整體天線之虛部阻抗,對阻抗頻寬有較劇烈之影響。最後固定參數:L 1= 8.2 nH、L 2= 10 nH、C 1= 3.3 pF,探討參數G為寄生短路之短路徑(CF)尾端與淨空區(421)邊界之間的間距(G),如第十一圖參數G反射損失變化圖,當參數G在0.8 mm變化至0.2 mm,同樣為寄生短路之短路徑(CF)所共振之低頻帶第二模態及倍頻的高頻帶第二模態有影響,此現象是很合理的。 The parameters will be discussed and analyzed for Proposed Antenna. First fixed parameters: L 2 = 10 nH, C 1 = 3.3 pF, G = 0.5 mm, and the parameter L 1 is the first inductance component (L1) of the high-pass matching circuit, as shown in the eighth figure parameter L 1 reflection loss variation diagram, When the parameter L 1 changes from 7.2 nH to 9.2 nH, since L 1 is a high-pass matching circuit component, the amount of inductance mainly affects the impedance bandwidth of the low frequency, which also confirms that the high-pass matching circuit described above mainly controls the low-band portion. Then fixed parameters: L 1 = 8.2 nH, C 1 = 3.3 pF, G = 0.5 mm, and the parameter L 2 is the second inductance element (L2) in the short path (CF) of the parasitic short circuit, as shown in the ninth parameter L 2 reflection loss variation map, when the parameter L 2 changes from 8 nH to 12 nH, it can be observed that the frequency of the second mode of the low frequency band will obviously move to the low frequency, and the short path of the parasitic short circuit (CF) is added by the second inductance. The component (L2) has to shorten the resonance wavelength and can resonate in the low frequency band with a shorter path, but the inductance should not be too large, otherwise the radiation efficiency of the antenna will be affected. Fixed parameters: L 1 = 8.2 nH, L 2 = 10 nH, G = 0.5 mm. Exploring parameter C 1 is the capacitive element C1 of the high-pass matching circuit, as shown in the tenth parameter C 1 reflection loss change diagram, when the parameter C 1 is 1.3 pF changes to 5.3 pF, because the capacitive component C1 is placed in the feedband unipolar path (AD), it will affect the imaginary impedance of the overall antenna, which has a strong impact on the impedance bandwidth. The last fixed parameter: L 1 = 8.2 nH, L 2 = 10 nH, C 1 = 3.3 pF, and the parameter G is the distance between the short path (CF) end of the parasitic short circuit and the boundary of the clearance area (421) (G) , as shown in the eleventh figure, the parameter G reflection loss change graph, when the parameter G changes from 0.8 mm to 0.2 mm, the short-path (CF) of the parasitic short-circuit is also the low-band second mode and the multi-frequency multi-band The two modes have an effect, and this phenomenon is very reasonable.

再由電流表面分佈圖來判斷模態之路徑,以及說明本發明之單極天線的物理特性,如第十二圖(a)、(b)、(c)、(d)、(e)為本發明之單極天線模擬電流圖。以下依序介紹頻率為715 MHz、778 MHz、859 MHz、1881 MHz及2562 MHz時模擬單極天線電流分布情形,上述頻率為輸入阻抗模態所匹配之頻率點,可了解到該模態所共振路徑長度。首先參照第十二圖(a)所示,當頻率為715 MHz時,可觀察到寄生短路之長路徑(CE)上是有較強的電流分佈,符合單極天線四分之一波長由強到弱之電流分佈,總路徑長度為67.7 mm(約為0.16λ),因為小尺寸天線路徑之間耦合影響而縮短共振路徑,導致共振長度不到四分之一波長,由上述結果可以證明在頻率715 MHz之模態是由寄生短路之長路徑(CE)所共振之主模態;第十二圖(b)所示,當頻率為778 MHz時,較強的電流分佈是集中在寄生短路之短路徑(CF)上,由於在寄生短路之短路徑(CF)中有加入一第二電感元件(L2)可以縮短模態共振路徑長度,總路徑長度為47.5 mm(約為0.12λ),由上述結果可以證明在頻率778 MHz之模態是由寄生短路之短路徑(CF)所共振之主模態;第十二圖(c)所示,當頻率為859 MHz時,可觀察到較強的電流分佈是集中在高通匹配電路內之第一電感元件(L1)上,由上述結果可以證明第一電感元件(L1)接地後是可以共振在頻率859 MHz之模態;第十二圖(d)所示,當頻率為1881 MHz時,由於此模態為寄生短路之長路徑(CE)所共振之倍頻模態,較強的電流分佈是集中在寄生短路之長路徑(CE)上,在電流分佈上會有反向電流零點產生,總路徑長度為67.7 mm(約為0.43λ);最後如第十二圖(e)所示,當頻率為2562 MHz時,由於此模態為寄生短路之短路徑(CF)所共振之倍頻模態,所以可以觀察到,較強的電流分佈是集中在寄生短路之短路徑(CF)上,在電流分佈上亦有反向電流零點產生,同樣是倍頻模態會產生之物理效應,總路徑長度為47.5 mm(約為0.4λ)。The current surface profile is used to determine the path of the modality, and the physical characteristics of the monopole antenna of the present invention are illustrated, as shown in Fig. 12 (a), (b), (c), (d), (e). The monopole antenna of the present invention simulates a current map. The following describes the current distribution of the analog monopole antenna at frequencies of 715 MHz, 778 MHz, 859 MHz, 1881 MHz, and 2562 MHz. The above frequencies are the frequency points matched by the input impedance mode, and the resonance of the mode is known. Path length. Referring first to Figure 12(a), when the frequency is 715 MHz, a strong current distribution is observed on the long path (CE) of the parasitic short circuit, which is consistent with the quarter-wavelength of the monopole antenna. To the weak current distribution, the total path length is 67.7 mm (approximately 0.16λ), because the resonance path is shortened due to the coupling effect between the small-sized antenna paths, resulting in a resonance length of less than a quarter wavelength, which can be proved by the above results. The mode at 715 MHz is the dominant mode of resonance by the long path (CE) of the parasitic short circuit; as shown in Fig. 12(b), when the frequency is 778 MHz, the strong current distribution is concentrated on the parasitic short circuit. On the short path (CF), the modal resonant path length can be shortened by adding a second inductive component (L2) in the short path (CF) of the parasitic short circuit, and the total path length is 47.5 mm (about 0.12λ). From the above results, it can be proved that the mode at the frequency of 778 MHz is the main mode of resonance by the short path (CF) of the parasitic short circuit; as shown in the twelfth figure (c), when the frequency is 859 MHz, the comparison can be observed. The strong current distribution is concentrated on the first inductive component (L1) in the high-pass matching circuit. As a result, it can be proved that the first inductance element (L1) is modal after being grounded at a frequency of 859 MHz; in the twelfth diagram (d), when the frequency is 1881 MHz, the modal is a long path of parasitic short circuit. (CE) The frequency doubling mode of resonance, the strong current distribution is concentrated on the long path (CE) of the parasitic short circuit, and there is a reverse current zero point in the current distribution, and the total path length is 67.7 mm (about 0.43λ); Finally, as shown in the twelfth figure (e), when the frequency is 2562 MHz, since this mode is the frequency doubling mode of the short path (CF) of the parasitic short circuit, it can be observed that The strong current distribution is concentrated on the short path (CF) of the parasitic short circuit. There is also a reverse current zero point in the current distribution. It is also the physical effect of the frequency doubling mode. The total path length is 47.5 mm (about 0.4λ).

如第十三圖(a)-(e)所示,為本發明之單極天線在中心頻率為740 MHz、925 MHz、1795 MHz、2045 MHz及2500 MHz時的模擬及實測2D輻射場型圖,在八個操作頻帶中心頻率中取五個中心頻率去觀察,低頻帶中心頻率740 MHz及925 MHz,高頻帶中心頻率1795 MHz、2045 MHz及2500 MHz,低頻部份X-Y平面有典型單極天線全向性輻射場型,而高頻部份場型上會有許多場型零點,由此可知,若天線操作波長小於系統接地面尺寸時(即操作頻率愈高),天線於接地面上表面電流零點也就相對較多,輻射場型則相對有較多的凹陷零點產生,此外也發現,輻射場型並沒有完全對稱,因天線元件(2)擺放位置,是在相對於整體接地元件(1)之第二表面(42)上方右側的淨空區(421),天線主體也非對稱性結構,所以得到非對稱性輻射場型之結果。As shown in Figures 13(a)-(e), the simulated and measured 2D radiation pattern of a monopole antenna of the present invention at center frequencies of 740 MHz, 925 MHz, 1795 MHz, 2045 MHz, and 2500 MHz Five center frequencies are observed in the center frequency of the eight operating bands, the low-band center frequencies are 740 MHz and 925 MHz, the high-band center frequencies are 1795 MHz, 2045 MHz and 2500 MHz, and the low-frequency part XY plane has a typical monopole antenna. Omnidirectional radiation field type, and there are many field zeros on the high frequency part field. It can be seen that if the antenna operating wavelength is smaller than the system ground plane size (ie, the higher the operating frequency), the antenna is on the ground plane surface. The current zero point is relatively more, and the radiation field type has relatively more concave zero points. In addition, it is also found that the radiation field type is not completely symmetrical, because the antenna element (2) is placed in position relative to the whole grounding element. (1) The clearance area (421) on the right side above the second surface (42), the antenna body is also asymmetric, so that the result of the asymmetric radiation pattern is obtained.

第十四圖為本發明之單極天線模擬及實測增益圖,第十五圖為本發明之單極天線模擬及實測輻射效率圖。由第十四圖、十五圖可以觀察到本天線較佳實施例操作在低頻LTE700/GSM850/900頻帶時,其天線增益介於0.2-1.4 dBi,且天線效率約為42-53%,而操作於高頻GSM1800/1900/UMTS/LTE2300/2500時,其天線增益介於3.4-4.3 dBi,且天線效率約為70-85%,本發明之單極天線設計的特性表現已符合實際應用之要求。Figure 14 is a diagram showing the simulated and measured gain of the monopole antenna of the present invention. The fifteenth figure is a simulation diagram of the simulated and measured radiation efficiency of the monopole antenna of the present invention. It can be observed from the fourteenth and fifteenth views that the preferred embodiment of the present antenna operates in the low frequency LTE700/GSM850/900 frequency band, and the antenna gain is between 0.2 and 1.4 dBi, and the antenna efficiency is about 42-53%. When operating at high frequency GSM1800/1900/UMTS/LTE2300/2500, the antenna gain is between 3.4-4.3 dBi and the antenna efficiency is about 70-85%. The performance of the monopole antenna design of the present invention has been adapted to practical applications. Claim.

以上所舉者僅係本發明之部份實施例,並非用以限制本發明,致依本發明之創意精神及特徵,稍加變化修飾而成者,亦應包括在本專利範圍之內。The above is only a part of the embodiments of the present invention, and is not intended to limit the present invention. It is intended to be included in the scope of the present invention.

綜上所述,本發明實施例確能達到所預期之使用功效,又其所揭露之具體技術手段,不僅未曾見諸於同類產品中,亦未曾公開於申請前,誠已完全符合專利法之規定與要求,爰依法提出發明專利之申請,懇請惠予審查,並賜准專利,則實感德便。In summary, the embodiments of the present invention can achieve the expected use efficiency, and the specific technical means disclosed therein have not been seen in similar products, nor have they been disclosed before the application, and have completely complied with the patent law. The regulations and requirements, the application for invention patents in accordance with the law, and the application for review, and the grant of patents, are truly sensible.

(1)‧‧‧接地元件(1)‧‧‧ Grounding components

(2)‧‧‧天線元件(2) ‧‧‧Antenna components

(21)‧‧‧第一輻射單元(21)‧‧‧First Radiation Unit

(211)‧‧‧電路元件組(211)‧‧‧Circuit component group

(212)‧‧‧L形延伸部(212) ‧‧‧L-shaped extension

(22)‧‧‧第二輻射單元(22) ‧‧‧second radiating element

(221)‧‧‧鉤狀延伸部(221)‧‧‧Hook extension

(222)‧‧‧C形延伸部(222)‧‧‧C-shaped extension

(3)‧‧‧金屬邊框部(3)‧‧‧Metal frame department

(31)‧‧‧第一L形金屬部(31)‧‧‧First L-shaped metal parts

(32)‧‧‧第二L形金屬部(32)‧‧‧Second L-shaped metal parts

(33)‧‧‧U形金屬部(33)‧‧‧U-shaped metal parts

(4)‧‧‧基板(4) ‧‧‧Substrate

(41)‧‧‧第一表面(41) ‧‧‧ first surface

(42)‧‧‧第二表面(42) ‧‧‧second surface

(421)‧‧‧淨空區(421)‧‧‧ clearance area

(A)‧‧‧饋入點(A) ‧ ‧ feed points

(B)‧‧‧端點(B) ‧‧‧ endpoint

(C)‧‧‧端點(C) ‧ ‧ endpoints

(E)‧‧‧第二自由端(E) ‧ ‧ second free end

(D)‧‧‧第一自由端(D) ‧ ‧ first free end

(F)‧‧‧第三自由端(F) ‧ ‧ third free end

(G)‧‧‧間距(G) ‧‧‧ spacing

(H)‧‧‧第四自由端(H) ‧ ‧ fourth free end

(L1)‧‧‧第一電感元件(L1)‧‧‧First Inductive Component

(L2)‧‧‧第二電感元件(L2)‧‧‧second inductance component

(C1)‧‧‧電容元件(C1)‧‧‧Capacitive components

(AD)‧‧‧饋入帶單極路徑(AD)‧‧‧Feed with unipolar path

(CE)‧‧‧寄生短路之長路徑(CE) ‧‧‧Long path of parasitic short circuit

(CF)‧‧‧寄生短路之短路徑(CF) ‧‧‧ Short path of parasitic short circuit

第一圖:本發明之應用於具有金屬邊框之電子裝置的LTE多頻單極天線的結構示意圖First: Schematic diagram of the structure of an LTE multi-frequency monopole antenna applied to an electronic device having a metal frame according to the present invention

第二圖:本發明之應用於具有金屬邊框之電子裝置的LTE多頻單極天線的結構局部放大示意圖FIG. 2 is a partially enlarged schematic view showing the structure of an LTE multi-frequency monopole antenna applied to an electronic device having a metal frame according to the present invention;

第三圖:本發明之單極天線結構模擬與實際量測反射損失圖The third figure: the single pole antenna structure simulation and actual measurement reflection loss map of the present invention

第四圖:本發明之單極天線結構模擬反射損失圖Figure 4: Simulated reflection loss diagram of the monopole antenna structure of the present invention

第五圖:為Antenna-1模擬輸入阻抗圖;(a)頻率響應圖;(b)與(c)史密斯圖Figure 5: Analog input impedance map for Antenna-1; (a) frequency response map; (b) and (c) Smith chart

第六圖:為Antenna-2模擬輸入阻抗圖;(a)頻率響應圖;(b)與(c)史密斯圖Figure 6: Analog input impedance map for Antenna-2; (a) frequency response map; (b) and (c) Smith chart

第七圖:Antenna-3模擬輸入阻抗圖;(a)頻率響應圖;(b)與(c)史密斯圖Figure 7: Antenna-3 analog input impedance map; (a) frequency response map; (b) and (c) Smith chart

第八圖:參數L1反射損失變化圖Figure 8: Parameter L 1 reflection loss change diagram

第九圖:參數L2反射損失變化圖Figure IX: Parameter L 2 reflection loss change diagram

第十圖:參數C1反射損失變化圖Figure 10: Parameter C 1 reflection loss change graph

第十一圖:參數G反射損失變化圖Figure 11: Parameter G reflection loss change diagram

第十二圖(a):當頻率為715 MHz時,本發明之單極天線模擬電流圖Twelfth Figure (a): Simulated current diagram of the monopole antenna of the present invention at a frequency of 715 MHz

第十二圖(b):當頻率為778 MHz時,本發明之單極天線模擬電流圖Twelfth Figure (b): Simulated current diagram of the monopole antenna of the present invention when the frequency is 778 MHz

第十二圖(c):當頻率為859 MHz時,本發明之單極天線模擬電流圖Twelfth Figure (c): Simulated current diagram of the monopole antenna of the present invention when the frequency is 859 MHz

第十二圖(d):當頻率為1881 MHz時,本發明之單極天線模擬電流圖Twelfth Figure (d): Simulated current diagram of the monopole antenna of the present invention when the frequency is 1881 MHz

第十二圖(e):當頻率第十二圖為本發明之單極天線模擬電流圖為2562 MHz時,本發明之單極天線模擬電流圖Twelfth Figure (e): When the frequency twelfth figure of the present invention is an analog current diagram of a monopole antenna of 2562 MHz, the monopole antenna analog current diagram of the present invention

第十三圖(a):本發明之單極天線在中心頻率為740 MHz時的模擬及實測2D輻射場型圖Thirteenth Figure (a): Simulated and measured 2D radiation pattern of a monopole antenna of the present invention at a center frequency of 740 MHz

第十三圖(b):本發明之單極天線在中心頻率為925 MHz時的模擬及實測2D輻射場型圖Thirteenth Figure (b): Simulated and measured 2D radiation pattern of a monopole antenna of the present invention at a center frequency of 925 MHz

第十三圖(c):本發明之單極天線在中心頻率為1795 MHz時的模擬及實測2D輻射場型圖Thirteenth Figure (c): Simulated and measured 2D radiation pattern of a monopole antenna of the present invention at a center frequency of 1795 MHz

第十三圖(d):本發明之單極天線在中心頻率為2045 MHz時的模擬及實測2D輻射場型圖Thirteenth (d): Simulated and measured 2D radiation pattern of a monopole antenna of the present invention at a center frequency of 2045 MHz

第十三圖(e):本發明之單極天線在中心頻率為2500 MHz時的模擬及實測2D輻射場型圖Thirteenth (e): Simulated and measured 2D radiation pattern of a monopole antenna of the present invention at a center frequency of 2500 MHz

第十四圖:本發明之單極天線模擬及實測增益圖Figure 14: Simulation and measured gain diagram of the monopole antenna of the present invention

第十五圖:本發明之單極天線模擬及實測輻射效率圖Figure 15: Simulation and measured radiation efficiency diagram of the monopole antenna of the present invention

(2)‧‧‧天線元件 (2) ‧‧‧Antenna components

(21)‧‧‧第一輻射單元 (21)‧‧‧First Radiation Unit

(22)‧‧‧第二輻射單元 (22) ‧‧‧second radiating element

(3)‧‧‧金屬邊框部 (3)‧‧‧Metal frame department

(31)‧‧‧第一L形金屬部 (31)‧‧‧First L-shaped metal parts

(32)‧‧‧第二L形金屬部 (32)‧‧‧Second L-shaped metal parts

(33)‧‧‧U形金屬部 (33)‧‧‧U-shaped metal parts

(4)‧‧‧基板 (4) ‧‧‧Substrate

(41)‧‧‧第一表面 (41) ‧‧‧ first surface

(42)‧‧‧第二表面 (42) ‧‧‧second surface

(421)‧‧‧淨空區 (421)‧‧‧ clearance area

Claims (9)

一種應用於具有金屬邊框之電子裝置的LTE多頻單極天線;至少包含一接地元件、一天線元件及一金屬邊框部;   所述接地元件位於一基板的第一表面,相對所述第一表面的所述基板的第二表面上設所述天線元件,所述金屬邊框部位於所述基板的周邊;   所述天線元件包含第一輻射單元及第二輻射單元;所述第一輻射單元包括彼此連接延伸的一電路元件組以及一L形延伸部,所述L形延伸部遠離所述電路元件組的一端為第一自由端;所述電路元件組包含一第一電感元件與一電容元件,所述電容元件的一端為天線訊號饋入點並與所述接地元件連接,所述電容元件的另一端連接所述第一電感元件與所述L形延伸部,所述電感元件的另一端連接所述接地元件;   所述第二輻射單元與所述接地元件連接,並至少具有C形延伸部與鉤狀延伸部,所述C形延伸部及所述鉤狀延伸部分別具有第三自由端及第四自由端,所述C形延伸部及所述鉤狀延伸部之間連接有第二電感元件,所述鉤狀延伸部設一端點與所述接地元件連接,所述鉤狀延伸部之端點與所述第四自由端之間形成開口,應用於具有金屬邊框之電子裝置的LTE多頻單極天線所述L形延伸部由所述開口深入所述鉤狀延伸部,所述鉤狀延伸部之末端和所述金屬邊框部連接,所述C形延伸部的自由端係位在所述第二輻射單元與所述接地元件連接處的一側;   所述金屬邊框部包括第一L形金屬部、第二L形金屬部及U形金屬部,所述第一L形金屬部、所述第二L形金屬部及所述U形金屬部係包圍設置在所述基板周圍。An LTE multi-frequency monopole antenna applied to an electronic device having a metal frame; comprising at least one grounding element, an antenna element and a metal frame portion; the grounding element is located on a first surface of a substrate opposite to the first surface The antenna element is disposed on a second surface of the substrate, the metal frame portion is located at a periphery of the substrate; the antenna element includes a first radiating unit and a second radiating unit; and the first radiating unit includes each other Connecting a circuit element group and an L-shaped extension portion, wherein an end of the L-shaped extension away from the circuit component group is a first free end; the circuit component group includes a first inductance component and a capacitance component, One end of the capacitive element is an antenna signal feed point and is connected to the ground element, and the other end of the capacitive element is connected to the first inductance element and the L-shaped extension, and the other end of the inductance element is connected The grounding element; the second ejector unit is coupled to the grounding element and has at least a C-shaped extension and a hook-shaped extension, the C-shaped extension And the hook-shaped extensions respectively have a third free end and a fourth free end, and the second inductive element is connected between the C-shaped extension and the hook-shaped extension, and the hook-shaped extension has an end point Connecting with the grounding element, an opening is formed between an end of the hook-shaped extension and the fourth free end, and the L-shaped extension is applied to an LTE multi-frequency monopole antenna having an electronic device with a metal frame The opening extends deep into the hook-shaped extension, the end of the hook-shaped extension is connected to the metal frame portion, and the free end of the C-shaped extension is tied to the second radiation unit and the ground element a side of the joint; the metal frame portion includes a first L-shaped metal portion, a second L-shaped metal portion, and a U-shaped metal portion, the first L-shaped metal portion, the second L-shaped metal portion, and The U-shaped metal portion is surrounded by the substrate. 如申請專利範圍第1項所述之應用於具有金屬邊框之電子裝置的LTE多頻單極天線,其中,所述第二輻射單元自與所述接地元件連接之端點至所述第四自由端之路徑,再經由連接的所述第一L形金屬部之第二自由端以激發出第一模態。An LTE multi-frequency monopole antenna for use in an electronic device having a metal frame as described in claim 1, wherein the second radiating element is from an end point connected to the ground element to the fourth free The end path is further excited by the second free end of the connected first L-shaped metal portion to excite the first mode. 如申請專利範圍第2項所述之應用於具有金屬邊框之電子裝置的LTE多頻單極天線,其中,所述第二輻射單元延伸自與所述接地元件連接之端點至所述C形延伸部之第三自由端之路徑以激發出第二模態。An LTE multi-frequency monopole antenna for use in an electronic device having a metal frame as described in claim 2, wherein the second radiating element extends from an end point connected to the ground element to the C-shape A path of the third free end of the extension to excite the second mode. 如申請專利範圍第3項所述之應用於具有金屬邊框之電子裝置的LTE多頻單極天線,其中,所述饋入點至第一電感元件連接所述接地元件之路徑以激發出第三模態。An LTE multi-frequency monopole antenna for use in an electronic device having a metal frame as described in claim 3, wherein the feeding point to the path of the first inductive element connecting the ground element to excite a third Modal. 如申請專利範圍第4項所述之應用於具有金屬邊框之電子裝置的LTE多頻單極天線,其中,所述第二輻射單元延伸自所述接地元件之端點至第四自由端之路徑再經由連接的所述第一L形金屬部之第二自由端以激發出第四模態,所述第四模態之頻率為所述第一模態之頻率的三倍。An LTE multi-frequency monopole antenna for use in an electronic device having a metal frame as described in claim 4, wherein the second radiating element extends from an end of the ground element to a path of the fourth free end And passing through the second free end of the connected first L-shaped metal portion to excite a fourth mode, the fourth mode having a frequency that is three times the frequency of the first mode. 如申請專利範圍第5項所述之應用於具有金屬邊框之電子裝置的LTE多頻單極天線,其中,所述第二輻射單元延伸自所述接地元件之端點至所述C形延伸部之第三自由端之路徑以激發出第五模態,所述第五模態之頻率為所述第一模態之頻率的三倍。An LTE multi-frequency monopole antenna for use in an electronic device having a metal frame as described in claim 5, wherein the second radiating element extends from an end of the ground element to the C-shaped extension The third free end path elicits a fifth mode, the fifth mode having a frequency that is three times the frequency of the first mode. 如申請專利範圍第6項所述之應用於具有金屬邊框之電子裝置的LTE多頻單極天線,其中,由所述饋入點至所述第一自由端之路徑以激發出第六模態。An LTE multi-frequency monopole antenna for use in an electronic device having a metal frame as described in claim 6, wherein a path from the feed point to the first free end is used to excite a sixth mode . 如申請專利範圍第7項所述之應用於具有金屬邊框之電子裝置的LTE多頻單極天線,其中,所述第一模態、所述第二模態及所述第三模態共同涵蓋687 MHz至960 MHz頻帶,所述第四模態、所述第五模態及所述第六模態共同涵蓋1675 MHz至2696 MHz頻帶。An LTE multi-frequency monopole antenna for use in an electronic device having a metal frame as described in claim 7, wherein the first mode, the second mode, and the third mode together In the 687 MHz to 960 MHz band, the fourth mode, the fifth mode, and the sixth mode collectively cover the 1675 MHz to 2696 MHz band. 如申請專利範圍第1至8項中任意一項所述之應用於具有金屬邊框之電子裝置的LTE多頻單極天線,其中,所述第一L形金屬部與所述第二L形金屬部對應,所述U形金屬部的二端分別與所述第一L形金屬部、所述第二L形金屬部相鄰且各形成一第一間距、第二間距,所述第一間距、第二間距距離相等,所述第一L形金屬部與所述第二L形金屬部間形成第三間距。An LTE multi-frequency monopole antenna applied to an electronic device having a metal frame according to any one of claims 1 to 8, wherein the first L-shaped metal portion and the second L-shaped metal Correspondingly, the two ends of the U-shaped metal portion are respectively adjacent to the first L-shaped metal portion and the second L-shaped metal portion and each form a first pitch and a second pitch, and the first spacing The second pitch distance is equal, and a third pitch is formed between the first L-shaped metal portion and the second L-shaped metal portion.
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